Breaking vectors into components — the key to 2D forces, motion, and fields
A vector A with magnitude A and angle θ from +x axis:
Aˣ = A cos θ Aʸ = A sin θ
Conversely: A = √(Aˣ² + Aʸ²), θ = tan⁻¹(Aʸ/Aˣ)
A = Aˣî + Aʸĵ (î = unit vector in x, ĵ = in y)
This makes addition trivial: just add î components and ĵ components separately.
| Quantity | Symbol | Component Form |
|---|---|---|
| Displacement | Δr | Δx î + Δy ĵ |
| Velocity | v | vₓ î + vʸ ĵ |
| Acceleration | a | aₓ î + aʸ ĵ |
| Force | F | Fₓ î + Fʸ ĵ |
| Momentum | p | pₓ î + pʸ ĵ |
| Electric Field | E | Eₓ î + Eʸ ĵ |
Three forces act on an object: F₁ = 10 N at 0°, F₂ = 15 N at 90°, F₃ = 20 N at 210°. Find net force.
F₁ˣ = 10 cos0° = 10, F₁ʸ = 10 sin0° = 0
F₂ˣ = 15 cos90° = 0, F₂ʸ = 15 sin90° = 15
F₃ˣ = 20 cos210° = 20(-√3/2) = -17.3, F₃ʸ = 20 sin210° = 20(-½) = -10
Rˣ = 10 + 0 - 17.3 = -7.3 N
Rʸ = 0 + 15 - 10 = 5 N
R = √((-7.3)² + 5²) = √(53.3+25) = √78.3 = 8.85 N
θ = tan⁻¹(5/-7.3) = tan⁻¹(-0.685) = -34.4° + 180° = 145.6° (QII)
Projectile launched at 30 m/s, 40°. Find vₓ, vᵧ. After 2s, find velocity components (g=10).
v₀ₓ = 30 cos40° = 23.0 m/s
v₀ᵧ = 30 sin40° = 19.3 m/s
vₓ(2s) = 23.0 m/s (constant, no air resistance)
vᵧ(2s) = v₀ᵧ - gt = 19.3 - 20 = -0.7 m/s (descending)
Speed = √(23.0² + 0.7²) = 23.0 m/s
Angle = tan⁻¹(-0.7/23.0) = -1.7° (slightly below horizontal)
Block on 30° incline, m=5kg, μ=0.2. Find acceleration using vector components.
Choose axes: x down incline, y perpendicular to incline.
Weight components: Wₓ = mg sin30° = 50 × 0.5 = 25 N
Wᵧ = -mg cos30° = -50 × (√3/2) = -43.3 N
Normal force: Nᵧ = +43.3 N (cancels Wᵧ)
Friction: f = μN = 0.2 × 43.3 = 8.66 N (opposes motion, so -x direction)
Net Fₓ = 25 - 8.66 = 16.34 N
aₓ = Fₓ/m = 16.34/5 = 3.27 m/s²
1) (a) 43.3î+25ĵ (b) 50î+86.6ĵ (c) -141î-141ĵ 2) R=5î+35ĵ, R=35.4, θ=81.9° 3) Zero (symmetric!)
4) v₀=(16.1,19.1); t=1: (16.1,9.1); t=3: (16.1,-10.9) 5) R=36.1N, θ=112.6° 6) 13, -67.4° (or 292.6°) 7) √34≈5.83 m/s, tan⁻¹(5/3)≈59° N of E